When we differentiate a power of , we bring the power down and reduce it by .
When we integrate, we do the reverse – first increase the power by , then divide by the new power on the outside.
Things don’t change when you have a negative exponent:
This holds true for fractions as well. When you do have fractional powers in a more involved integral, things can become a bit more difficult to spot.
And of course, it holds for irrationals too…
So generally, for any real 1
Power rule crops up everywhere in integration, since it’s a really fundamental integration method. The most important cases are where and .
This looks really obvious, but when you’ve just started integration, it can be easy to forget what you’re doing when the variables change after a substitution. Always remember that it doesn’t matter what you call your integrating variable – , , , they’re all just labels – the methods remain the same.
For , you’re just integrating a constant, and this gives back your integrating variable:
It probably feels a bit weird at first integrating ‘nothing’. Just remember you’re not integrating , but . If you really want, you can explicitly write the in:
[!Tip] Integrating just gives , since any constant differentiates to . For that we’d explicitly write .
Ok, are there any real values of that power rule doesn’t hold for? There is, actually. We reach a strange case with as the exponent:
If we try applying power rule, we would increment the power to (giving , a constant) – but more catastrophically, we’d end up dividing by …
Which is definitely illegal.
This is actually the 1 special case where the power rule doesn’t hold. So can be any real number except . We’ll look at how to integrate next in Integrating the Reciprocal.
- *Except , as we’ll soon see.↩